Treating Ocular Refractive Error

ABSTRACT

A lens for an eye that includes a zone with a first power profile for images received by the retina on the fovea, a zone with a second power profile for images received by the peripheral retina on the nasal side and a zone with a third power profile for images received by the peripheral retina on the temporal side. The first power profile is selected to provide clear or acceptable vision and the second and third power profiles are selected to affect the peripheral image position.

RELATED APPLICATION

This application claims the benefit of Australian patent application2010903334 filed on 26 Jul. 2010, the entire content of which isIncorporated herein by reference.

FIELD OF THE INVENTION

The invention generally relates to methods and devices for treatingrefractive error in an eye, Particular embodiments may have applicationto influencing the rate of progression of refractive error, by slowingthe progression of refractive error and/or preventing the progression ofrefractive error. Particular embodiments may have application to thecontrol of progression of myopia. Other embodiments may have applicationto the control of the progression of hyperopia.

BACKGROUND

Myopia (short-sightedness) is a disorder of the eye in which distantobjects cannot be clearly focused, but near objects can be. Images ofdistant objects are brought to focus in front of the retina; that is,the focusing power of the eye is too strong ‘at distance’. The conditionmay be corrected by the use of a negatively powered lens, which causesthe distant Images to focus on or nearer the fovea. Myopia can be aserious and progressive condition that leads to increasing visualimpairment despite the use of corrective lenses. It is becomingincreasingly common, with some countries in South-East Asia reportingthat 80% of children aged 17 years suffer from the condition.

Hyperopia (long-sightedness) is a disorder where distant objects can befocused, but near objects cannot be focused. Hyperopia may be correctedby the use of positive power lenses.

It is generally agreed that the process of normal eyedevelopment—emmetropization—is regulated by a feedback mechanism, whichregulates the length of the eye to maintain good focus both at distanceand at near or emmetropia. While it is also generally agreed that thisfeedback mechanism is somehow disturbed in eyes with refractive error,so that the eye grows too long In myopia and not long enough inhyperopia, there has not been consensus about the nature of the feedbackmechanism or how the progression of myopia and hyperopia can becontrolled. Both biochemical and optical (focal defect) mechanisms havebeen suggested.

While it is generally assumed that the feedback stimulus is somehowrelated to focal defects of the eye, the matter cannot be simplebecause, in progressive myopia, the condition may become worse—i.e., theeye continues to lengthen excessively—even though lenses that correctfor distance vision are worn.

It has been proposed that an optical feedback mechanism is somehow upsetby deficiencies in the accommodative effort of the eye due to excessivenear work. The deficiency is considered to manifest as lag ofaccommodation (imprecise and insufficient accommodation) in some myopiceyes at near, resulting in defocus, which stimulates further undesirableaxial elongation of the eye.

Bifocal lenses and PALS (progressive addition lenses) in spectacles havebeen proposed as a possible way to relieve the accommodative stress anddefocus in the hope that the stimulus for elongation would be removed.U.S. Pat. No. 6,752,499 (Alter) describes prescribing commerciallyavailable bifocal contact tenses for myopic eyes that also exhibit nearpoint esophoria to control the progression of myopia. Both concentricdistance center and near center contact lenses were employed in myopiceyes with near point esofixation disparity. The zones of the concentricdistance and near zones lie within the pupil.

In U.S. Pat. No. 6,045,578 (Collins et al.) it is proposed thatemmetropization is regulated by the degree and direction of a sphericalaberration present at the fovea. It is proposed that young myopes havehigher levels of negative spherical aberration that promotesinappropriate eye growth and that the use of ophthalmic lenses to Impartpositive spherical aberration will counteract axial growth and thus theprogression of myopia.

In international patent publication number WO 200604440A2 (Phillips etal) it is proposed that defocus at the fovea for both distance and nearvision inhibits the feedback stimulus for excessive eye growth. Thispublication proposes the use of a bi-focal contact lens thatsimultaneously provides the central retina with (a) clear vision forboth distance and near and (b) myopic defocus for both distance andnear. Again, the visual image will be degraded if this proposal is used.

U.S. Pat. No. 7,025,460 (Smith et al) describes the results of animaltrials demonstrating that it is the optical state of the peripheralretina, not the fovea, that dominates the feedback stimulus foremmetropization. Thus, Smith et al, proposes that controlling off-axisfocal points of the eye relative to the central on-axis focal pointsthrough manipulation of the curvature of field of the visual imageprovides a method of abating, retarding or controlling the progressionof myopia and hypermetropia (impaired near vision caused by Insufficienteye length).

FIGS. 1 and 2 show how Smith et al describe an eye 1 that has a positivecurvature of field. Since the central on-axis image point 2 is locatedin front of (i.e. opposite to the direction of light) the retina 3, thiseye is considered myopic when measured using standard techniques such asauto-refractors, refractor-heads or trial frames, in the manner thateye-care practitioners are familiar. In this representative eye, theoff-axis peripheral image points 4 for large field angles are locatedbehind (i.e. in the direction of light) the retina 3. Thus the eye 1 ofthis example is relatively hypermetropic for the peripheral visualfield. FIG. 2 shows a relative field curvature graph for the eye 1,which shows that the central to mid-peripheral field 5 is myopic (focusin front of retina 3) but the mid-peripheral to far-peripheral field 6Is hypermetropic (focus behind retina 3).

FIGS. 3 and 4 show how the eye 1 of FIGS. 1 and 2 is prescribed anoptical device 7 for the control of the progression of myopia, asdescribed by Smith et al. This optical device 7 is designed so that itwould generate a negative relative curvature of field 8 on the eye 1.The central, on-axis image 9 is focused sharply to the fovea 11 enablinggood visual acuity. The optical device 7 introduces sufficient negativerelative curvature of field 8 to focus the peripheral image points 13more anteriorly, or in front (i.e. in the direction against thedirection of light in the eye) of the retina 3.

U.S. Pat. No. 7,665,842 (Ho at al) describes providing one or morevision priority zones in which peripheral defocus or another aberrationis corrected, with the lens also controlling the relative curvature offield for the peripheral retina in another region outside of the visionpriority zone(s).

There remains a need for methods and optical devices that address thesuggested optical (focal defect) mechanisms of progression of refractiveerror, particularly in relation to the progression of myopia.

SUMMARY

The present invention relates to the utilization of the finding thatrefraction in central and peripheral areas of the retina of human eyes,or at least the eyes of a substantial or significant number of people,is such that the natural curvature of field of the visual image isasymmetric around the visual axis of the eye. In more detail, theinvention relates to the control of off-axis focal points of the eyerelative to the on-axis focal points in an asymmetric manner through theuse of an optical device that controls refraction of light for the eye.

For a patient with myopia, a method of treatment may therefore includemeasuring the refractive characteristics of the eye at the fovea (inother words on-axis or at the central retina) and outside the fovea (inother words off-axis or at the peripheral retina). The myopic patientmay then be treated by modifying the refractive properties of the ocularsystem to provide clear or acceptable vision on-axis and to control theposition of the image at the peripheral retina, for example to move theimage onto or in front of the retina. For an eye with asymmetry in theperipheral retina, a device to move the image at the peripheral retinawill require different refractive powers to treat the asymmetry observedin different parts of the peripheral retina. For a patient withhyperopia, the peripheral images may be moved onto or behind the retina,again treating for observed asymmetry in the eye.

One way of modifying the refractive properties is through the use of alens. Embodiments of a device for an eye include contact lenses,spectacle lenses, corneal implants or other lenses that have differentpower profiles for images received by different parts of the peripheralretina. The class of contact lenses includes lenses that operate byhaving a refractive power and orthokeratology lenses that achieve achange in the refractive properties of the eye by reshaping the cornea.

In some embodiments a lens is provided for affecting the progression ofmyopia or hyperopia in an eye. The lens comprises a nasal optic zone anda temporal optic zone for refracting light to be received by theperipheral retina. The nasal optic zone and temporal optic zone havedifferent refractive powers. The lens may further include a centraloptic zone with a refractive power to correct for the refractive powerof the eye on-axis and to provide clear or acceptable distance vision atall distances.

The lens may therefore comprise regions for affecting light destined tovarious sectors of the retina in a rotationally asymmetric mannerrelative to the central on-axis focal points. The lens may affect theperipheral light rays received by the retina of the patient's eye in anygiven sector so that their focal points are on or anterior to thesurface of the retina for myopes, or on or posterior to the surface ofthe retina for hyperopes. In this way, for at least some patients, thestimulus for aberrant eye growth may be removed in substantially allsectors or over an increased amount of the retina. The removal ofstimulus may be performed especially in those regions deemed to be ofmost importance for inhibiting such eye growth.

In some embodiments a method of prescribing an optical device foraffecting images received by the peripheral retina includes observingwhether the recipient of the optical device has a symmetrical orasymmetrical curvature of field. The prescribed optical device may theneither treat the peripheral image symmetrically or asymmetricallydependent on the observation.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1 and 2 (prior art) show a previous diagrammatic description of aneye with positive curvature of field.

FIGS. 3 and 4 (prior art) show how the curvature of field of the eyerepresented by FIGS. 1 and 2 may be manipulated using an optical device.

FIG. 5 shows a plot illustrating the asymmetry in the nasal versustemporal peripheral retina for a sample group of eyes of children withmyopia.

FIGS. 6 to 9 show example structures of a contact lens for eyes withasymmetry between the nasal and temporal fields.

FIG. 10 shows a flow chart of a method for treating an eye with anoptical device including a lens.

FIGS. 11 to 13 show an instrument for obtaining on-axis and off-axisrefractive measurements of an eye.

DESCRIPTION

FIG. 5 shows a plot of the refractive state for 1155 eyes of childrenwith myopia at the peripheral retina in the horizontal meridian, withmeasurements for the both the nasal and temporal quadrants taken. Thehorizontal (independent) axis indicates the peripheral angles at whichmeasurements were taken. Measurements at the nasal retina represent thetemporal visual field and measurements at the temporal retina representthe nasal visual field. The vertical (dependent) axis is the amount ofdefocus of the light rays at the retina, in diopters (D), relative tothe amount of defocus along the visual axis of the eye. Accordingly,positive values Indicate relative hyperopic defocus and negative valuesrelative myopic defocus. Measurements of defocus were taken on axis andat 20, 30 and 40 degrees from the optical axis, both temporally andnasally. The eyes had a spherical equivalent refractive error of−2.27±0.81D on axis. All measurements were taken using an open fieldShin Nippon autorefractor utilizing head-turn for off-axis measurementsso the eyes were in the primary position for all measurement angles. Theplot was completed by simple straight line interpolation between themeasured points.

FIG. 5 shows that at 20 degrees, the nasal retina is experiencing 0.43 Dof hyperopic defocus relative to central retina. In contrast, thetemporal retina is experiencing only 0.14D of hyperopic defocus relativeto the central retina. At 30 degrees, the amount of hyperopic defocusexperienced by the nasal retina increases to 0.92D relative to centralretina and the temporal retina experiences 1.08D. At 40 degrees, thehyperopic defocus experienced by the nasal retina increases to 1.64Dcompared to central retina. At the temporal retina, there is asignificant increase in the hyperopic defocus and increases to 2.47Drelative to central retina.

FIG. 5 shows that whilst there may be relative hyperopic defocusexperienced at both the nasal and temporal retina relative to thecentral retina, the amount of defocus experienced at each point measuredvaries and is asymmetric around the central on axis image point. FIG. 5also shows the standard deviation of the measured relative defocus ateach measurement angle for the same set. For some eyes in the sampleset, the asymmetry was such that there was relative myopic defocus onone side of the peripheral retina and relative hyperopic defocus on theother side.

The measurement of the eye, as represented by the plot in FIG. 5 differssubstantially from the representation described in U.S. Pat. No.7,025,460 (Smith et al), which assumes the curvature of field of thiseye is rotationally symmetric relative to the central on-axis imagepoint. Thus, the manipulation of the curvature of the field in asymmetric fashion, as taught in U.S. Pat. No 7,025,460 (Smith et al), isunlikely to eliminate the defocus in all quadrants of an eye havingcharacteristics shown in FIG. 5 and may be under-correcting orover-correcting for either the hyperopic or myopic defocus present in atleast some locations of the peripheral retina.

Accordingly, the present invention involves modifying the wavefront oflight received by an eye by creating an ocular system including the eyethat takes into account asymmetry in the curvature of field of the eyeto be treated. In other words, if the relative curvature of field wascontrolled in a symmetrical manner, then the peripheral image wouldremain asymmetrical, however if the asymmetry of the eye is taken intoaccount, this asymmetry can be reduced or eliminated. This allowsplacement of the image substantially on the retina on both the nasal andtemporal sides of the fovea. Alternatively, this allows thesubstantially symmetrical profile shown in FIG. 4 to be achieved for amyopic eye, despite asymmetry in the refractive characteristics of theeye for peripheral images. Similarly, for a hyperopic eye, takingaccount of the asymmetry can result in a treated eye havingsubstantially symmetrical characteristics or at least reduced asymmetry.

FIGS. 6 to 9 show examples of the general structure of four differentcontact lenses 100, 200, 300, 400, for controlling the relative positionof peripheral images of an eye with asymmetric relative curvature offield in the horizontal direction. Each lens is for a left eye andgenerally has a different refractive power in a region on the nasal sideto that on the temporal side. A design for the right eye may be mirrorimage in structure, but the power profile in each optic zone will beselected dependent on the characteristics of the right eye. Each lenshas an optic zone 101, 201, 301, 401, which may be between approximately6 to 8 mms in diameter, depending on the particular implementation.Outside the optic zone 101, 201, 301, 401 is a carrier portion 102, 202,302, 402, which provides stability for the lens when applied to the eye.The carrier portion may for example extend for another 4 to 6 mm, sothat the total lens diameter up to the lens edge 106, 206, 306, 406 maybe about 12 mm. Other embodiments may have differing dimensions, andparticular dimension lenses may in some cases be selected according tothe eye to which the lens is to be applied, for example to reflectdifferences in size of the pupil 50. In FIGS. 6 to 9 the outer peripheryof the carrier zone is represented in dashed lines.

The lenses are each oriented on the eye with the utilization of asuitable lens stabilization technique. The requirement to stabilize theorientation of the lens arises since the power of the contact tensvaries across the surface and is effected to ensure application of powerto selected regions of the central and the peripheral regions of theretina. The lenses may be stabilized on eye with a lens stabilizingmechanism selected from a prism ballast, double slab-off and truncation.

For the representative eye plotted In FIG. 5, between the field anglesof 20 to 40 degrees, the temporal peripheral retina is experiencing 0.14to 2.4D of relative hyperopic defocus and the nasal peripheral retina isexperiencing 0.43 to 1.64D of relative hyperopic defocus. The followingdescription of the lens structures shown in FIGS. 6 to 9 assumes thatthe power profile of the optic zones in the contact lens is designedwith this defocus, in mind.

In the example shown in FIG. 6, the lens 100 has a disc-shaped centraloptic zone 103. The central optic zone 103 has a diameter selected fromthe range of from about 0.5 mm up to about 3 mms. The central optic zone103 is located and provided with a power to correct for the centralrefractive error of the eye (measured at the fovea). With this selectionof power, the central optic zone 103 allows for clear vision at alldistances (assuming that the eye can accommodate to provide in focusnear vision). The power profile of the lens varies between the nasaloptic zone 104 and temporal optic zone 105 on either side of the centraloptic zone 103. The power in these zones is selected to correct for thedefocus measured In the temporal and nasal quadrants of the peripheralrespectively.

In some embodiments, these zones may carry a single power that correctsfor the average defocus measured at the peripheral retina over a rangeof field angles. Thus for example, in these embodiments the nasal opticzone 104 will correct for the mean 1.23D of relative hyperopic defocusexperienced by the peripheral retina on the temporal side and thus willbe 1.23D relatively more positive compared to the power of the centraloptic zone 103. Similarly, the temporal optic zone 105 will correct forthe mean 0.99D of relative hyperopic defocus experienced by theperipheral retina on the nasal side and thus will be 0.99D relativelymore positive compared to central optic zone power.

In other embodiments, the nasal and temporal optic zones 104, 105 carrya plurality of powers, selected with regard to the defocus measured attwo or more locations of the peripheral retina. For example, the powerof the nasal optic zone may be set taking account of the relativedefocus experienced by the temporal peripheral retina at 20, 30 and 40degrees and include a smooth transition between the powers required atthese angles. If measurements are taken for an eye at more angles or atonly two angles, then the power may be set in the nasal and temporaloptic zones 104, 105 having regard to those measurements. The variationmay reflect the measured curvature of field of the eye to which the lensis to be applied. For example, a lens may be selected with a powerprofile across the nasal optic zone 104 that has the objective of asubstantially constant distance (which may be zero) between the focalpoint and the retina. Similarly variations in power may occur across thetemporal optic zone.

The options of having either a single power in a zone or a varying powerin a zone also applies to the lens structures shown in FIGS. 7 to 9.

In the example shown in FIG. 7, the lens 200 has a central optic zone203 extending along the vertical meridian of the lens 200. The centraloptic zone 203 has a constant power from the centre to the periphery ofthe optic zone in both directions. The width of the meridian is in therange from about 0.5 mm to about 3 mms. The power profile of the lens200 varies between the nasal optic zone 204 and temporal optic zone 205on either side of the central zone 203 and will correct for the defocusmeasured for the peripheral retina on the temporal and nasal sidesrespectively, as described for the example shown in FIG. 6.

In the example shown in FIG. 8, the lens 300 has a central optic zone303 between approximately 0.5 mm to 3 mm in diameter with a refractivepower selected to correct for the central refractive error of the eye.In the horizontal meridian, the power profile of the lens 300 variesbetween the nasal and temporal optic zones 304, 305 on either side ofthe central optic zone 303, as described for the example shown in FIG.6. The nasal and temporal optic zones 304, 305 have a height ofapproximately 0.5 mm to 3 mm, which may be selected to match thediameter of the central optic zone 303, although in other embodimentsthe height of these zones may be more or less than the diameter of thecentral optic zone 303. The nasal and temporal optic zones 304, 305 bothextend from the central optic zone 303 to the edge of the optic zone 301of the lens 300. The central optic zone 303 is extended into the regions307, 308 outside of the peripheral optic zone. In other words, in thisexample, in the optic zone 301, the lens 300 has a power selected tocorrect for the central refractive error of the eye in all regionsoutside of the nasal and temporal optic zones 304, 305.

In the example shown in FIG. 9, the lens 400 has a central optic zone403 between approximately 0.5 to 3 mm in diameter that corrects for thecentral refractive error. In the horizontal meridian, the power profileof the lens varies between the nasal and temporal optic zones 404, 405on either side of the central optic zone 403. The nasal temporal zone404 and temporal optic zone 405 correct for the defocus measured in thetemporal and nasal quadrants of the peripheral retina respectively, asdescribed above with reference to the example shown in FIG. 6. Both thenasal and temporal optic zones 404, 405 have an oblong shape of width ofabout 3.0 mm to 5.0 mm. These zones need not be oblong and could beother shapes, like circular or substantially rectilinear. The remainderof the lens carries the same power profile as the central optic zone.

For each of the examples shown in FIGS. 6 to 9, there may be atransition zone connecting the central optical zone (and any otherregion with the same power profile as the central optic zone) to theperipheral optic zones (consisting of the nasal and temporal opticzones). The transition zone is at the boundary of the central and nasalor temporal optic zones and can vary in width from about 0.25 mm toabout 1.0 mm. The transition zone bridges the difference in powerprofile and In some embodiments is shaped to provide a smooth curvetransition between the zones. In other embodiments, there may be a pointon the lens where the central optical zone finishes and the peripheraloptic zone commences.

As will be appreciated from the description herein, including but notlimited to the examples shown in FIGS. 6 to 9, the shape and layout ofthe optic zones in a contact lens may be varied substantially, creatinga large range of different embodiments. By way of example; the centraloptic zone 103, 203, 303, 403 may be asymmetrical about a verticalmeridian of the lens through the centre of the lens. This asymmetry mayreflect a low rate of change in the curvature of field for one side ofthe peripheral retina. Referring to FIG. 5, the rate of change betweenzero to twenty degrees for the temporal retina is low, so that someembodiments of lens may have a power selected to correct on-axis visionfor these field angles. If the eye already has the desired or anacceptable curvature of field on one side, the central optic zone may beextended to encompass the entirety of what would otherwise be thetemporal optic zone (or the nasal optic zone). Each embodiment howeverremains characterized by different power profiles in a nasal optic zoneand a temporal optic zone, selected to control the off-axis focal pointsof the eye relative to the central on-axis focal points in an asymmetricmanner.

The lens power profile may not consider the refractive error state ofthe eye in the vertical direction, as differences along verticalmeridians are not considered as important. However, in otherembodiments, the refractive error state of the eye in the verticaldirection may also be corrected, in the same way as described herein forthe horizontal direction. In other words, the relative curvature offield naturally occurring In the eye in the vertical direction may alsobe measured and the lens may include upper and lower optic zones tocontrol the curvature of field for the lower and upper potions of theperipheral retina respectively. Where there is asymmetry in the verticaldirection, this may be accounted for in the same manner as asymmetry inthe horizontal direction. Where both the horizontal and verticaldirections are controlled, the peripheral image will be controlled inall quadrants of the eye.

The examples shown in FIGS. 6 to 9 show a central optic zone 103, 203,303, 403. In the examples, a central optic zone of diameter or width ofabout 0.5 to 3.0 mm is provided. The size of the central optic zone maybe selected regarding to the pupil diameter of the recipient of the lensor having regard to the average pupil diameter of a population samplemost representative of the recipient or a sample representing thegeneral population. Generally, a larger central optic zone allows forclearer vision, particularly if the central optic zone has a constant orsubstantially constant power profile across the area of the pupil.However, a lens with a smaller central optic zone may be required forsome recipients where control of peripheral defocus close to the foveais needed. Some sacrifice of on axis image quality may then result.

Also, the central optic zone 103, 203, 303, 403 may have a power profileselected to correct on-axis vision, with a substantially uniform poweracross its diameter In all directions. Having a central optic zone maybe advantageous in minimizing defocus of the image received by thefovea. In other embodiments, the power profile of the central optic zonemay be allowed to vary to some extent. For example, the lens may bedesigned to have a power profile that progressively changes from thecentre point of the lens out to the nasal and temporal optic zones. Thepower at the centre point of the lens may be selected to correct on-axisvision, or selected to provide substantially clear vision on axis.

The contact lenses shown in FIGS. 6 to 9 may be silicone hydrogellenses, rigid lenses, scleral lenses or hybrid lenses. Similar lensdesigns may be made for spectacle lenses and corneal implants. For boththese types of lenses the carrier portion is not required. A suitablestructure for spectacle lenses may be that shown in FIG. 9, except witha central optic zone of a width of about 8 to 20 mm. Some embodiments ofspectacle lens may have a large transition zone between the centraloptic zone and the peripheral optic zone, so as to avoid visible lineson the lenses and to reduce interference with the clarity of vision ofthe wearer when their eyes are not directed straight ahead. Cornealimplants will be shaped to create a conreal surface profile that resultsin the refractive characteristics described. An orthokeratology lens maysimilarly reshape the cornea to achieve the relative curvature of fieldrequired for the peripheral retina.

A collection of lenses may be provided from which a selection is madefor individual recipients. For example, for each power in the centraloptic zone, there may be a selection of asymmetric peripheral opticzones. The selection may be made with reference to a population norm andthe deviation for the population, for example as represented in FIG. 5.Where there a significant variations in classes of recipients, differentpopulation norms may be constructed for each class. The number ofselections for each power in the central optic zone may vary. Oneexample may be a selection of: one for the average for the populationfour for the standard deviation either side (which takes into accountthat a eye with relatively more myopic defocus in comparison to the normon one side of the peripheral retina may my more myopic or morehyperopic in comparison to the norm on the other side of the peripheralretina) and another four at 1.5 standard deviation. Additional lensesmay be available for one or more of: 0.25 of the standard deviation, 0.5of the standard deviation, 0.75 of the standard deviation and 2.0standard deviations. It will be appreciated that some of the lenses Inthe collection may be symmetrical or substantially symmetrical, whichmay be selected for appropriate recipients. There may be selections forthe power profile of the central optic zone and/or the structure (forexample two of more of the structures shown in FIGS. 6 to 9) as well.

FIG. 10 shows a flow diagram of a series of steps for prescribing a lensfor the correction of refractive error of an eye with the purpose ofalso attempting to control the change in refractive error over time. Instep 1000 a patient is identified with refractive error. Thisidentification step may be achieved by a simple examination of thehistory of on-axis refractive error of a patent, for example over thepast 6 months or 1 to 3 years, or longer. Alternatively, theIdentification step 1000 may be replaced with identification of apatient that has refractive error without reference to any history oferror or its progression.

In step 1001 the on-axis refractive error is measured. This measurementis used to identify the required correction on-axis. For example, thepatient may be measured as having refractive error of −3 D, in whichcase the central optic zone of the lens, for example the central opticzone 103, 203, 303, 403 shown in FIGS. 8-9 is selected to have a powerto correct this error.

In step 1002 the off-axis refractive error is measured. Measurements aretaken for off-axis field angles nasally and temporally. As previouslydescribed, variation in field of curvature for vertical angles may beignored, but may be measured and included in the lens design ifrequired. Step 1002 may comprise taking a measurement at a single anglein the nasal and temporal directions, for example at 30 degrees relativeto the on-axis direction. Alternatively, step 1002 may comprise takingmeasurements at more than one angle in the nasal and temporaldirections. For example two measurements may be taken at 15 and 30degrees, three measurements taken at 15, 30 and 35 degrees or sixmeasurements taken at 5, 10, 15, 20, 25 and 30 degrees. The angle neednot be a multiple of five, these angles being described for illustrativepurposes only. More than one measurement may be taken at a single angleand these may be combined, for example through averaging or otherwise ormay be subject to evaluation, for example with reference to the positionof the eye when the measurement was taken, with the measurement expectedto be the most accurate selected.

Depending on the instrument used, step 1002 may include separate stepsfor measuring the refractive characteristics of an eye at each requiredangle relative to the optical axis of the eye. For example, this may berequired if the patient has to be physically moved or asked to movetheir line of sight, or if the instrument needs to be physically movedrelative to the patient's eye to obtain the measurements.

In step 1003 the measurements are compared to available lenses withdiffering power across the horizontal meridian for the best match, or anew lens design is formed for manufacture with the required powerprofile for the eye. The power profile corrects for the on-axisrefractive error measured in step 1000 in the central optic zone and hasa power selected with regard to the refractive characteristics of theeye in the nasal and temporal peripheral regions.

For example, the power profile may be selected to place the image ofperipherally viewed objects on the retina in both the nasal and temporaldirections, or on the retina for at least those angles which have beenmeasured in step 1002. Alternatively, where there are constraints on thepower profile across the lens, the power profile may be selected toplace the image of peripherally viewed objects as close as possible tothe retina within those constraints. The constraints may include aconstraint on the maximum rate of change or constraints due torequirements to correct other conditions, such as astigmatism.

Alternatively, the power profile may be selected to place the image ofperipherally viewed objects at another position relative to the retina,where that is viewed as potentially providing benefit. For example, fora myopic eye, the power profile may be selected to place the image ofperipheral objects in front of the retina. For a hyperopic eye, thepower profile may place the image of peripheral objects behind theretina. The objective for placement of the image of peripheral objectsneed not be symmetrical—for example the lens for a myopic eye may placethe peripheral image on the temporal side on the retina and theperipheral image on the nasal side in front of the retina.

The refractive state of the eye, both on-axis and for peripheralobjects, is measured using retinoscopy. Either manual or autorefractorsmay be used to take the measurements. An example of an instrumentspecifically designed for measuring both on axis and peripheralrefraction will now be described.

FIGS. 11 and 12 show an instrument 10 suitable for measuring peripheralrefraction, determining the amount of decentration and applying acorrection factor to obtain a corrected measurement of peripheralrefraction. The present invention may be implemented In software in thecontroller 49 (see FIG. 12). The apparatus, together with possiblevariations of the instrument 10 and alternative apparatus that may beadapted to implement the current invention is described in internationalpatent publication PCT/AU2008/000434, published as WO 2008/116270 A1,the content of which is incorporated herein in its entirety byreference. The instrument 10 uses the general methodology of ‘instrumentrotation’ described in relation to FIG. 2. Other instruments with whichthe present may be implemented may use the ‘eye turn’ or ‘head turn’methodologies.

FIG. 11 shows the basic layout of the instrument 10. An array 12 ofdeflector elements 14 is in this example instrument a linear row thatextends symmetrically and laterally on either side of the optical axis16 of the eye-related optical system 18 under investigation. It will beassumed that system 18 is the eye of a patient with or without theaddition of prosthetic lenses or other modifications. An illuminatinglight source, controlling processor and return-beam detector areindicated by a single undifferentiated unit 20 arranged on axis 16,which is described In more detail with reference to FIG. 3. Unit 20directs illuminating beams, indicated by arrow heads 22, to arrayelements 14 to generate a corresponding set of interrogating beams,indicated by arrow heads 24, that are directed into eye-system 18 atdifferent peripheral angles relative to axis 16. A return beam,indicated by arrow heads 23, is generated by each interrogating beam 24and is directed back to unit 20 via the respective element 14 fordetection. It is convenient for illuminating beams 22 to be directed insequence from one element 14 to the next to thereby sequentiallygenerate the interrogating beams 24 and return beams 23.

In this example, a central illuminating beam, a corresponding centralinterrogation beam and a corresponding central return beam are indicatedby arrow heads 25, 27 and 29. Also in this example, each deflectorelement is a prism (except central element 14 c) that has an apex anglesuch that each interrogation beam 24 is directed into eye 18 and eachreturn beam 23 is directed to unit 20. Central element 14 c iseffectively a null element that does not deflect the illuminating beam;it may be a parallel-sided plain glass as shown, but that is not evennecessary. Also in this example, array 12 is substantially linear sothat interrogating beams 24 and 27 are substantially co-planar allowingone meridian—the horizontal In this example—of system 18 to beinvestigated. Non-horizontal meridians of the system can be investigatedby simply rotating the instrument 10 about optic axis 16 relative to eye18.

The transmission of Interrogating beams 24 and 27 one at a time into eye18, and the generation of a corresponding sequence of return beams 23and 29, can be effected in a variety of ways. First (as will bedescribed below), unit 20 may include a beam scanner that directs asingle narrow illuminating beam from one element 14 to another. Second,multiple elements 14 can be illuminated at one time and interrogatingbeams 24 and 27 can be gated to effect scanning of eye 18 and thegeneration of a sequence of return beams 23 and 25. This can be done by,for example, inserting an electronically controllable LCD shutter 26between array 12 and eye 18 and using it as scanning means by whichinterrogating beams 24 from prisms 14 are admitted into eye 18 one at atime. Third, a similar shutter 28 may be inserted between array 12 andunit 20 to gate illuminating beams 22 and 25 to illuminate one or moreelements 14 at a time. Thus, it is not essential for unit 20 to includescanning means and it is possible to distribute the scanning functionbetween scanner means in unit 20 and shutters such as indicated at 26and/or 28

In this way, successive interrogation/retum beam pairs diverge/convergeat successively larger/smaller angles with respect to axis 16 as theypass into and out of eye 18. Sequential scanning from one angle to thenext adjacent will probably be most convenient but many other scansequences may be used to minimise biases that might arise due to fixedsequential scanning. While illumination of more than one beam deflectorelement 14 at a time can easily be achieved by use of a scanner in unit20, it is then necessary to distinguish the multiple simultaneous returnbeams that will result. This can be done by using shutter 26 or 28 as abeam-chopper or selective polariser to differentially encode each returnbeam that needs to be distinguished from another at the detector.

FIG. 12 is a more detailed side elevation of instrument 10 of FIG. 11 inwhich the principal components of unit 20 are shown separately. A lightsource 30 directs a collimated source beam 32 via a beam-splitter 34 toan oscillating mirror scanner 36 that is moved by actuator 37 togenerate illuminating beams 22. The illuminating beans 22 are scannedfrom deflector to deflector in array 12 to generate the sequence ofinterrogating beams 24 that are directed into the eye-system 18 and ontothe retina 38 over the desired range of incident angles. Scanning mirror36 thus forms a point source or common point for beams 24 and a commonpoint (indicated at X) for all return beams. Thus, each return beam 23returned from retina 38 passes back via deflector array 12 and scannermirror 36 to beam-splitter 34 by which it is diverted via a focusingsystem 42 to a photo detector 44. System 42 includes a moveable lensassembly 43 that can be moved axially back and forth through a focusrange, as indicated by arrows 46. While the source beam 32 (and, thus,the illuminating, interrogating and return beams 22, 24 and 23) can haveany desired spot, disc or annular cross-section desired, an annularcross-section like that commonly used in known autorefractors (such theShin-Nippon SRW-5000 mentioned above) is preferred as it can be analysedand processed in a substantially standard manner.

Each return beam 23—or more correctly its image 48 at detector 44 thuscontains information of the (uncorrected for decentration) refractivestatus of the eye-system that is captured or quantified by the photodetector 44, which is preferably a two-dimensional array of photosensors. The photo detector 44 also captures an image of the pupilcorresponding to the image shown in FIG. 7 for the determination of thedecentration of the illuminating beams 22. An image of the pupil iscaptured when each refraction measurement is made, so that there is oneimage for each illuminating beam 22. This allows the refractionmeasurement to be individually corrected at each incident angle, dealingwith relative movement of the eye-system 18 and the measurement axisbetween measurements.

The unit 20 includes a central processor and controller 49 that mayconveniently comprise a dedicated PC and is connected to accept andanalyse the output of detector 44 and to drive lens assembly 43 underservo-control. Processor 49 is also connected to control scanner driver37 and to ensure correct timing of illumination and return signaldetection. A connection between light source 30 and processor 49 is alsoshown as it will be convenient to ensure that source beam 32 iscorrectly configured and that a representation of the current sourcebeam sectional pattern is stored for comparison with image 48.

While each return beam 23 is being received, focusing lens assembly 42is moved along the direction of the optical axis to vary the focus sizeand shape of the image 48. Commonly, three positions of the focusingassembly 42 are recorded for each of three return beam image shapes: oneposition where the image (spot or ring) appears smallest and in sharpestfocus, a second position where the image appears maximally elongated inone meridian and a third position where the image is maximally elongatedin a different meridian, usually one that is orthogonal to the firstmeridian. The three positions of lens assembly 42 respectively indicatethe spherical equivalent power of the eye, the sagittal astigmaticcomponent and the tangential astigmatic component of the refraction. Thesignificance of spot/image size in relation to spherical equivalentpower of eye 18 can be understood in the following elementary way. Sincethe interrogating beam 24 that enters eye 18 is collimated, a normal oremmetropic eye will return a parallel collimated beam, a myopic eye willreturn a convergent beam and a hyperopic eye will return a divergentbeam, both of which will result in larger images sizes.

The central processor and controller 49 stores in memory the correctionalgorithm, either as a function or as a look-up table. It also includesinstructions to receive and/or automatically determine the decentrationand to apply the correction algorithm to the measured refraction valuesto calculate a corrected refraction value. The corrected refractionvalues may then be stored, displayed or communicated to another device.

FIG. 13 shows some features that may be added to enhance the performanceof the instrument 10 of FIGS. 13 and 14. A movable fixation target 50 islocated on a gaze beam path 52 that is optically coupled by a firstadditional beam-splitter 54 into return beam path 23 and on optical axis16. Fixation target 50 aligns the gaze or axis of the eye with opticalaxis 16 of the system and controls accommodation. A second additionalbeam-splitter 56 In gaze path 52 directs an image of eye 18 onto a CCDdetector 58, allowing gaze direction and eye-alignment to be monitoredsince CCD detector 58 receives the ocular image via beam-splitters 54and 56. Optical or acoustical distance sensors 60 can be used to(alternately or additionally) indicate when eye 18 appears to be axiallyaligned. Sensors 60, along with detector 58 if desired, can be connectedto processor 49 (FIG. 12)—as indicted by arrows marked P—so thatinitiation of a measurement cycle can be automatic.

It will be understood that the invention disclosed and defined in thisspecification extends to all alternative combinations of two or more ofthe individual features mentioned or evident from the text or drawings.All of these different combinations constitute various alternativeaspects of the invention.

1. A lens for an eye, the lens comprising a zone with a first powerprofile for images received by the retina on the fovea, a zone with asecond power profile for images received by the peripheral retina on thenasal side, a zone with a third power profile, different from at leastthe second power profile, for images received by the peripheral retinaon the temporal side, and a lens stabilizing mechanism for orienting thelens on the eye, wherein the first power profile is selected to provideclear or acceptable vision and the second and third power profiles areselected to affect the progression of refractive error. 2-3. (canceled)4. A lens for affecting the progression of myopia in an eye, the lenscomprising a nasal optic zone and a temporal optic zone for refractinglight to be received by the peripheral retina so as to be focused on orin front of the retina, wherein the nasal optic zone and the temporaloptic zone have different refractive powers.
 5. A lens for affecting theprogression of hyperopia in an eye, the lens comprising a nasal opticzone and a temporal optic zone for refracting light to be received bythe peripheral retina so as to be focused on or behind the retina,wherein the nasal optic zone and temporal optic zone have differentrefractive powers.
 6. The lens of claim 5 further comprising a centraloptic zone with a refractive power to correct on-axis vision of the eye.7. The lens of claim 5 wherein the nasal optic zone has an increasedpower relative to a power on-axis and the temporal optic zone has adecreased power relative to the power on-axis.
 8. The lens of claim 5wherein the temporal optic zone has an increased power relative to anon-axis power and the nasal optic zone has a decreased power relative tothe on-axis power.
 9. The lens of claim 5 further comprising a centraloptic zone between the nasal and the temporal optic zones, the centraloptic zone being asymmetrical about a vertical meridian through thelens, so as to extend across horizontal half meridians of the lens todifferent extents, wherein the vertical and horizontal meridians referto the orientation of the lens caused by a stabilizing mechanism. 10.The lens of claim 9, wherein the central optic zone is not plano andincludes a refractive power for correcting defocus.
 11. The lens ofclaim 5, wherein the nasal optic zone and the temporal optic zone bothinclude a substantially constant refractive power in a verticaldirection, wherein the vertical direction is with reference to theorientation of the lens caused by the stabilizing mechanism.
 12. Thelens of claim 5, wherein the nasal and temporal optic zones have avertical height of between 0.5 mm and 3 mm.
 13. The lens of claim 12,further comprising a central optic zone with a refractive power tocorrect on-axis vision of the eye, wherein the lens has a refractivepower substantially equal to the refractive power of the central opticzone above and below the nasal and temporal optic zones.
 14. The lens ofclaim 5, further comprising a central optic zone with a refractive powerto correct on-axis vision of the eye, wherein the central optic zone issubstantially rotationally symmetrical.
 15. The lens of claim 5, furthercomprising a central optic zone with a refractive power to correcton-axis vision of the eye, wherein the central optic zone is elongate ina vertical direction across the lens, wherein the vertical direction iswith reference to the orientation of the lens caused by a stabilizingmechanism.
 16. The lens of claim 15, wherein the lens is a contact lenswith an optic zone and a carrier and wherein the central optic zoneextends in the vertical direction across substantially the entire opticzone.
 17. The lens of claim 5, wherein one of the nasal optic zone andtemporal optic zone has a power selected to place peripheral images onthe retina and the other zone has a power selected to place peripheralimages off the retina. 18-20. (canceled)
 21. A method of treating an eyewith hyperopia comprising measuring the refractive characteristics ofthe eye at the central and peripheral retina to obtain on-axis andoff-axis measurements respectively, determining from said measuring thatthe eye has asymmetrical off-axis refractive characteristics andaffecting the refractive properties of an ocular system comprising theeye to provide clear or acceptable vision on-axis and to control theposition of the image of peripheral objects to onto or behind the retinaso as to also reduce said asymmetry for at least one off-axis angle. 22.The method of claim 21, wherein the ocular system comprises lens for theeye, the lens comprising a first zone with a first power profileselected to provide said clear or acceptable vision on-axis, a secondzone with a second power profile, which controls the position of theimage of peripheral objects received on the nasal side of the retina,and a third zone with a third power profile, which controls the positionof the image of peripheral objects received on the temporal side of theretina, wherein at least the second and third power profiles aredifferent so as to reduce said asymmetry.
 23. The method of claim 22,wherein the lens is a lens selected from the group comprising a contactlens and a spectacle lens.
 24. The method of claim 21, wherein the stepof affecting the refractive properties of an ocular system comprisingthe eye comprises applying an orthokeratology lens to the eye, theorthokeratology lens providing said clear or acceptable vision on-axisand controlling the position of the image of peripheral objects byreshaping the cornea.
 25. The method of claim 21, wherein the step ofaffecting the refractive properties of an ocular system comprising theeye comprises inserting a corneal implant into the eye, the cornealimplant providing said clear or acceptable vision on-axis andcontrolling the position of the image of peripheral objects by reshapingthe cornea.